vanhees71 said:
This is a very good example for why I thik that quantum states are better interpreted in an epistemic sense and why the collapse hypothesis leads to problems with locality and causality.
My view is that the correlations, as all probabilistic relations of quantum systems, are described by the state of the system, and the state of the system is determined by preparation. The preparation in that case is when the entangled photon pair is created (e.g., by parametric downconversion by shooting a laser beam into a crystal). When A measures her photon's polarization state (her photon is defined by that it is registered by the detector at A's place), she immediately also knows the polarization state of B's photon (his photon is defined by that it is registered by the detector at B's place, which can be very far distant from A's detector). For B nothing has changed. He simply expects an unpolarized photon and gets with 50% probability the one or the other polarization when he measures it.
Let's now assume that A's detector is very close to the photon source, and B's very far, such that A measures her photon earlier than B. In other words, the measurement processes are assumed to happen as time-like separated events. Then "collapse" happens definitely at different times for A than for B: A changes the state of the photon pair due to her measurement result much earlier than B. Still, there is no contradiction by what's known to A and B concerning the outcome of their mesaurements. Both A's and B's photons are exactly unpolarized, i.e., the polarization state if maximally indetermined.
There's, of course, also no problem when the measurement processes are realized at space-like distances. Then you can always find a reference frame, where A and B register their result simultaneously or another reference frame, where A registers her result before B or again another frame, where B registers his result before A. Still there's no contradiction, because both, A and B always just find that their photons sent from the source of entangled photon pairs are precisely unpolarized.
When A and B compare their measurement protocols (always keeping detailed track about the time, when they registered their measurement outcome to be sure to relate always the pairs which where created together at the source), they find in any case the 100% correlations due to the preparation of the photon pairs in the polarization-entangled state.
Of course, here I made two assumptions: (a) the polarization measurements are local events as described by standard QED and thus the linked-cluster principle is valid, i.e., A's measurement cannot instantaneously affect B's photon and/or measurement apparatus (implied by microcausality) and (b) that all there is possible to be known about photons is what is described by quantum states, and since this is probabilistic knowledge (some may think only) it refers to ensembles of equally prepared quantum systems, i.e., the probabilistic information described by the prepared state can only be tested by collecting "enough statistics", i.e., using a sufficiently large ensemble.
The problems start, whenever you try to give more meaning to the quantum state then is implied by this minimal interpretation. Some think (in the past Einstein and Schrödinger were the most prominent physicists to do so) that this is not a complete description of nature since "in reality" (whatever "reality" means to them) all possible observables should have determined values always. It's not completely ruled out that maybe somebody one day finds some satisfactory theory, where this is the case, but Bell's work and the empirical precise findings with respect to it, imply that such a deterministic hidden-variable theory must be non-local, and so far there seems not to be a satisfactory such kind of theory in the relativistic realm.
I still do not understand your position.
Supposing C performs a Bell's Inequality Test-like experiment. Where 2 photons are entangled and then separated.
Do you agree with the following QM assumptions:
1) The preparation would determine the correlation between the two, but not the polarisation of A or B's photon which would both be undetermined.
?
Imagine that the polarisation of photon A is then measured at detector A. Do you agree with the following assumption:
2) The polarisation of A and B's photon is given by the measurement (because of the correlation determined by the preparation), so they can no longer be considered undetermined.
?
Note these assumptions do not involve consideration of whether the polarisation of B was ever measured by a detector B, and so do not consider whether there was a spacelike or timelike separation between those measurements. But if you agree with those assumptions, then there is the issue of how the measurement of A's polarisation could have determined the polarisation of B's photon (consider a spacelike separation example).
Though regarding your view, you mention that A and B will find the correlation determined by the preparation process. But the issue is not about the correlation, but the polarisation value of B's photon. You mention that with spacelike separation A will know the polarisation of B's photon, but for B things are unchanged (in terms of what B knows). That B expects the polarisation result to still be 50/50, but so what. Suppose B is in the same rest frame as A and they have clocks synchronised in that rest frame, and that B's measurement takes place a second after A's by their clocks (still spacelike separation just quite far apart). And that later they meet up, and compare notes. Are you suggesting that if you were B upon meeting back up, and seeing the log of A's measurements you would be claiming that a millisecond prior to you making the measurement a second later (in the frame of reference you were both in) the result was undetermined and it was 50/50 what the result would be because you did not know what A had found out?
Regarding your point about the problem brought up with the standard relativity interpretation, in which even with spooky action at a distance, A's measurement determined B's polarisation to the same extent that B's determined A's (or whether they happened simultaneously), because which happened first was truly relative . That is an interpretation dependent issue. As I mentioned earlier Relativity is compatible with Presentism (the view that the set of what exists only contains entities that exist in the present) where one frame of reference (presumably) corresponds to the present, but there would likely be no way of establishing experimentally which one. With a Presentist interpretation, the determination issue disappears. It allows for either A's to have determined B's or B's to have determined A's, even if there was no experimental way of telling which way around it was, or for them to have happened simultaneously .
P.S. I do not know what the banned LET thing is. Checked for "LET physics" and found
https://en.wikipedia.org/wiki/Linear_energy_transfer, is that it? Or is it mentioning Presentism? If so I will avoid mentioning it again, though I would be interested in why it would be banned mentioning it, given that it is an interpretation that allows for a sequence of determination, and I am not sure why certain interpretations would be banned. Einstein seemed concerned with determination with his hidden variables vs dice idea, and some like MWI for its determination (though it has determination with no "spooky action at a distance"). If even asking about why it is banned is banned, could these last two paragraphs just be ignored.